Transparent p-type AlN:SnO2 and p-AlN:SnO2/n-SnO2:In2O3 p-n junction fabrication

Liu, Y. S.; Hsieh, Ching-Shieh; Wu, Yen‐Ju; Yu, Wei; Lee, P. M.; Liu, C. Y.

doi:10.1063/1.4754134

Cited by 27 publications

(19 citation statements)

References 26 publications

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“…Searching for exact solutions of nonlinear PDEs plays an important role in the study of these physical phenomena and gradually becomes one of the most important and significant tasks. In recent years, many direct methods for obtaining exact solutions of nonlinear PDEs have been presented, such as the tanh-function method [1][2][3], the homogeneous balance method [4], the sine-cosine method [5], the Jacobi elliptic function expansion method [6][7][8], the F -expansion method [9][10][11], the auxiliary equation method [12][13][14], and the exp-function method [15][16][17].…”

Section: Introductionmentioning

confidence: 99%

A transformed rational function method for (3+1)-dimensional potential Yu–Toda–Sasa–Fukuyama equation

Zhang

2011

Pramana - J Phys

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A direct method, called the transformed rational function method, is used to construct more types of exact solutions of nonlinear partial differential equations by introducing new and more general rational functions. To illustrate the validity and advantages of the introduced general rational functions, the (3+1)-dimensional potential Yu-Toda-Sasa-Fukuyama (YTSF) equation is considered and new travelling wave solutions are obtained in a uniform way. Some of the obtained solutions, namely exponential function solutions, hyperbolic function solutions, trigonometric function solutions, Jacobi elliptic function solutions and rational solutions, contain an explicit linear function of the independent variables involved in the potential YTSF equation. It is shown that the transformed rational function method provides more powerful mathematical tool for solving nonlinear partial differential equations.

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Section: Introductionmentioning

confidence: 99%

A transformed rational function method for (3+1)-dimensional potential Yu–Toda–Sasa–Fukuyama equation

Zhang

2011

Pramana - J Phys

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“…Normally, when TCOs are used as p-type and n-type defects easily form at the interface between the p-type TCOs and n-type TCOs, and they act as parallel resistances in the p-n junction, causing severe leakage current and a low turn-on voltage 20,21,[39][40][41][42]. The low leakage current and the turn-on voltage (3.24 V) approaching the bandgap of SnO 2 indicated that the defect level at the p-type AlN-doped SnO 2 /n-type fluorine-doped SnO 2 junction was low.…”

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confidence: 99%

Study of p-type AlN-doped SnO2 thin films and its transparent devices

Liu

Hsieh

et al. 2015

Applied Surface Science

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“…With a large mass, charmonium evolutions in the hot medium can be described by a classical Boltzmann transport equation. It has described well hadroproduced charmonium R AA (N p ) at different colliding energies from SPS to LHC [15,42,43], mean transverse momentum square p 2 T (N p ) [44], and rapidity distribution R AA (y) [16]. The transport equation for hadroproduced charmonium with cold and hot nuclear matter effects is…”

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confidence: 99%

“…F gΨ is the flux factor. Charmonium decay rate in QGP is proportional to the gluon thermal density f g (k, T ) and also their inelastic cross sections σ gΨ (T ) [44]. The cross section for gluon dissociation in vacuum σ gΨ (0) can be derived through the operator production expansion.…”

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confidence: 99%

Charmonium coherent photoproduction and hadroproduction with effects of quark gluon plasma

2018

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We study the charmonium coherent photoproduction and hadroproduction consistently with modifications from both cold and hot nuclear matters. The strong electromagnetic fields from fast moving nucleus interact with the other target nucleus, producing abundant charmonium in the extremely low transverse momentum region pT < 0.1 GeV/c. This results in significative enhancement of J/ψ nuclear modification factor in semi-central and peripheral collisions. In the middle pT region such as pT < 3 ∼ 5 GeV/c, J/ψ final yield is dominated by the combination process of single charm and anti-charm quarks moving in the deconfined matter, c +c → J/ψ + g. In the higher pT region, J/ψ production are mainly from parton initial hard scatterings at the beginning of nucleus-nucleus collisions and decay of B hadrons. We include all of these production mechanisms and explain the experimental data well in different colliding centralities and transverse momentum regions. 12.38.Mh, 24.85.+p With the nuclear collisions at the relativistic heavy ion collisions (RHIC) and the large hadron collider (LHC), there have been a lot of interesting topics about nuclear properties studied in experiments and theories. One of the main goals at RHIC and LHC is to find a deconfined state of nuclear matter, called "quark-gluon plasma" (QGP), which may be produced in the extremely high energy and/or baryon densities with a phase transition [1], and furthermore, extract the transport properties of this QGP [2]. There are also other projects referred to as "non-QGP " physics, concerning about cosmic ray physics and others [3]. As QGP can only be produced in the nucleon collisions in the overlap area of two nuclei, "non-QGP " topics are usually studied in Ultra-peripheral nuclear collisions (UPC) where QGP background is absent.In order to study the existence of the extremely hot deconfined matter, produced in the early stage of heavy ion collisions, J/ψ abnormal suppression has been proposed as one of sensitive signals by Matsui and Satz in 1986 [4]. J/ψ suffers relatively weaker dissociation by the hadron gas compared with QGP, due to its large binding energy [5]. With strong color screening effect and parton inelastic scatterings of QGP, J/ψ production can be significantly suppressed in nucleus-nucleus collisions, which has been observed in many experiments at RHIC and LHC colliding energies in semi-central and central collisions (with impact parameter b < 2R A , where R A is the nuclear radius) [6][7][8][9]. From RHIC to LHC, J/ψ production is relatively enhanced in the transverse momentum region p T ≤ 3 ∼ 5 GeV/c compared with the scale of the pp collisions [8]. This phenomenon has been well explained with charmonium regeneration mechanism: At higher colliding energy, more charm quark pairs can be produced from hard process in hadronic collisions, which enhance the recombination probability of charm and anti-charm quarks inside QGP [10][11][12][13][14]. New J/ψs are continuously regenerated during the QGP evolutions. With sufficiently high initial tem...

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Transparent p-type AlN:SnO2 and p-AlN:SnO2/n-SnO2:In2O3 p-n junction fabrication

Cited by 27 publications

References 26 publications

A transformed rational function method for (3+1)-dimensional potential Yu–Toda–Sasa–Fukuyama equation

A transformed rational function method for (3+1)-dimensional potential Yu–Toda–Sasa–Fukuyama equation

Study of p-type AlN-doped SnO2 thin films and its transparent devices

Charmonium coherent photoproduction and hadroproduction with effects of quark gluon plasma

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